Laser irradiation method, laser irradiation apparatus, and method of manufacturing a semiconductor device

ABSTRACT

In the present invention, each laser light emitted from a plurality of lasers is divided, and laser light including at least one laser light that is emitted from a different laser and that has different energy distribution is synthesized with another such laser light, or laser light including at least one laser light that has different energy distribution is synthesized with another such laser light through a convex lens that is set at an angle to the direction each laser light travels, to form laser light having excellent uniformity in energy distribution.

FIELD OF THE INVENTION

The present invention relates to a laser beam irradiation method and alaser irradiation apparatus for using the method (apparatus including alaser and an optical system for guiding laser beam emitted from thelaser to an object to be irradiated). In addition, the present inventionrelates to a method of manufacturing a semiconductor device, whichincludes a laser beam irradiation step. Note that a semiconductor devicedescribed here includes an electro-optical device such as a liquidcrystal display device or a light-emitting device and an electronicdevice that includes the electro-optical device as a part.

DESCRIPTION OF THE RELATED ART

In recent years, a wide study has been made on a technique in whichlaser annealing is performed for a semiconductor film formed on aninsulating substrate made of glass or the like, to crystallize the film,to improve its crystallinity so that a crystalline semiconductor film isobtained, or to activate an impurity element. Note that a crystallinesemiconductor film in this specification indicates a semiconductor filmin which a crystallized region is present, and also includes asemiconductor film that is crystallized as a whole.

A method of forming pulse laser beam from an excimer laser or the likeby an optical system such that it becomes a square shape or a linearshape on an irradiation surface, and scanning the laser beam (orrelatively shifting an irradiation position of the laser beam withrespect to the irradiation surface) to conduct annealing is superior inmass productivity and is excellent in technology. The “linear shape”described here means not a “line” in the strict sense but a rectangle(or a prolate ellipsoid shape) having a high aspect ratio. For example,it indicates a shape having an aspect ratio of 10 or more (preferably,100 to 10000). Note that the linear shape is used to obtain an energydensity required for sufficiently annealing an object to be irradiated.Thus, if sufficient annealing is conducted for the object to beirradiated, it may be either a rectangular shape or a planar. Presently,excimer lasers with 15 J/pulse come onto the market and there is apossibility to perform a laser anneal by a planar beam. Further, thespot of the laser light is made laser light's energy distribution on anirradiation surface of the laser light when there is not a specialdefinition.

FIG. 10 shows an example of a configuration of an optical system forforming laser beam in a linear shape on an irradiation surface. Thisconfiguration is extremely general. All optical systems described aboveare based on the configuration shown in FIG. 10. According to theconfiguration, a cross sectional shape of laser beam is converted into alinear shape, and simultaneously an energy density distribution of laserbeam on the irradiation surface is homogenized. In general, an opticalsystem for homogenizing the energy density distribution of laser beam iscalled a beam homogenizer.

The spot of the laser beam emitted from a laser 71 is divided by acylindrical lens array 73. The direction is called a first direction inthis specification. It is assumed that, when a mirror is inserted in acourse of an optical system, the above-mentioned first direction ischanged in accordance with a direction of light bent by theabove-mentioned mirror. In this configuration, the cylindrical lensarray is divided into seven parts. Then, the laser beams are superposedon an irradiation surface 79 by a cylindrical lens 74, therebyhomogenizing an energy density distribution of the linear laser beam inthe longitudinal direction, and the length of the longitudinal directionis determined.

Next, the configuration shown in the side view of FIG. 10 will bedescribed. The spot of the laser beam emitted from a laser 71 is dividedby cylindrical lens arrays 72 a and 72 b. The direction is called asecond direction in this specification. It is assumed that, when amirror is inserted in a course of an optical system, the seconddirection is changed in accordance with a direction of light bent by themirror. In this configuration, the cylindrical lens arrays 72 a and 72 beach are divided into four parts. The divided laser beams aretemporarily synthesized by a cylindrical lens 74. After that, the laserbeams are reflected by a mirror 77 and then condensed by a doubletcylindrical lens 78 so that they become again single laser beam on theirradiation surface 79. The doublet cylindrical lens 78 is a lenscomposed of two cylindrical lenses. Thus, an energy density distributionof the linear laser beam in a width direction is homogenized, therebyhomogenizing an energy density distribution of the linear laser beam inthe longitudinal direction, and the length of the width direction isdetermined.

For example, an excimer laser in which a size in a laser window is 10mm×30 mm (which each are a half-width in beam profile) is used as thelaser 71 and laser beam is produced by the optical system having theconfiguration shown in FIG. 10. Then, linear laser beam which has auniform energy density distribution and a size of 125 mm×0.4 mm can beobtained on the irradiation surface 79.

At this time, when, for example, quartz is used for all base materialsof the optical system, high transmittance is obtained. Note that coatingis preferably conducted for the optical system such that transmittanceof 99% or more is obtained at a frequency of the used excimer laser.

Then, the linear laser beam formed by the above configuration isirradiated with an overlap state while being gradually shifted in awidth direction thereof. Thus, when laser annealing is performed for theentire surface of an amorphous semiconductor film, the amorphoussemiconductor film can be crystallized, crystallinity can be improved toobtain a crystalline semiconductor film, or an impurity element can beactivated.

At an edge of linear, rectangular, or sheet-like laser light formed onan irradiation surface or in the vicinity thereof by an optical system,the energy density is attenuated gradually due to aberration of a lensor the like (FIG. 11A). In this specification, a region at a laser lightedge where the energy density is gradually attenuated is called anattenuation region.

As the substrate area is increased and the laser power is raised, it isnow possible to form a longer linear beam or rectangular beam and alarger sheet-like beam. Annealing with such laser light is moreefficient. However, the energy density of laser light emitted from alaser is smaller at its edge than around the center. Therefore, if laserlight is expanded by an optical system more than prior art, attenuationin the attenuation region is intensified.

In the attenuation region, the energy density is lower than a regionhaving a high uniformity in energy density and the low energy density isattenuated gradually. For that reason, an irradiation object cannot beannealed uniformly by laser light that has the attenuation region (FIG.11B). Even when the laser light scans an irradiation object forannealing in a manner that makes the attenuation regions overlap eachother, it still is impossible to anneal the irradiation object uniformlybecause annealing conditions of the attenuation region are entirelydifferent from annealing conditions of the highly uniform region.Accordingly, a region annealed by the attenuation region of laser lightand a region annealed by the highly uniform region of the laser lightcannot be treated equally.

For example, when a semiconductor film is an irradiation object, aregion of the semiconductor film that is annealed by the attenuationregion and a region of the semiconductor film that is annealed by thehighly uniform region have different crystallinity. Therefore, if thissemiconductor film varied in crystallinity from one region to another isused to manufacture TFTs, the electric characteristic of a TFT formedfrom the region that is annealed by the attenuation region is inferiorto other TFTs and causes fluctuation among the TFTs on the samesubstrate.

As shown in FIG. 10, a complicate optical system is needed to form alinear beam. Optical adjustment for an optical system as such is verydifficult to perform and, in addition, the apparatus has to be large insize because of large footprint.

If laser light used has high reflectance against an irradiation objectand the laser light enters the irradiation object perpendicular to theobject, the light goes back the light path it used upon entering theirradiation object (return light). Return light affects laser apparatusby changing the laser output and frequency and by breaking a rod.

SUMMARY OF THE INVENTION

The present invention has been made in view of the above, and an objectof the present invention is therefore to provide laser irradiationapparatus which uses a simpler optical system than prior art to form arectangular beam with the attenuation region at a laser light edgereduced for efficient annealing. Another object of the present inventionis to provide a laser irradiation method using this laser irradiationapparatus as well as a method of manufacturing a semiconductor devicewhich includes the laser irradiation method in its process.

The present invention is characterized in that laser beams emitted froma plurality of lasers are each divided and that laser beams emitted fromdifferent lasers and having different energy distributions aresynthesized to form laser light having excellent uniformity in energydistribution. Here, energy distributions which are not identical butbecome the same distribution by rotation are deemed as different energydistributions. Also, the present invention is characterized in thatlaser beams emitted from a plurality of lasers are each divided, andthat a laser beam including at least one laser beam that is emitted froma different laser and is in a different positional relation issynthesized with another such laser beam to form laser light havingexcellent uniformity in energy distribution.

Also, the present invention is characterized in that laser beams emittedfrom a plurality of lasers are each divided, and that laser beamsemitted from different lasers and having different energy distributionsenter a convex lens at an angle, exit the convex lens, and aresynthesized on an irradiation surface or in the vicinity thereof to formrectangular laser light having excellent uniformity in energydistribution.

Even when laser beams emitted from different lasers are overlapped, theydo not interfere each other. Accordingly the present invention iseffective especially for laser light irradiation that uses highlyinterferential lasers such as a YVO₄ laser having a coherent length ofseveral tens to several hundreds m and a YAG laser having a coherentlength of 1 cm or more.

By making laser light enter a convex lens at an angle, astigmatism orother aberration is caused to shape laser light into a linear shape onan irradiation surface or in the vicinity thereof.

When a divided laser beam is overlapped with another divided laser beam,it is preferred to overlap laser beams having different energydistributions from one another. This is because overlapping a largenumber of laser beams that have different energy distributions producesuniform laser light.

A structure of the present invention disclosed in this specification islaser irradiation apparatus characterized by comprising: a plurality oflasers; means for dividing each of plural first laser beams emitted fromthe plural lasers into plural second laser beams; and means for choosingone laser beam out of the second laser beams for each of the pluralfirst laser beams and synthesizing the chosen second laser beams in thesame region on an irradiation surface or in the vicinity thereof.

In the above structure, the laser irradiation apparatus is characterizedin that the lasers are continuous wave or pulse oscillation solid-statelasers or gas lasers or metal lasers. Examples of the solid-state lasersinclude a continuous wave or pulse oscillation YAG laser, YVO₄ laser,YLF laser, YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandritelaser, and Ti:sapphire laser. Examples of the gas lasers include acontinuous wave or pulse oscillation excimer laser, Ar laser, Kr laser,and CO₂ laser. Examples of the metal lasers include a continuous wave orpulse oscillation helium cadmium laser, copper steam laser, and goldsteam laser.

In the above structure, the laser light is desirably converted intoharmonic by a non-linear optical element. For example, a YAG laser isknown to output laser light having a wavelength of 1065 nm as thefundamental wave. This laser light is absorbed by a silicon film at avery low absorption coefficient and it is technically very difficult tocrystallize an amorphous silicon film, one of semiconductor films, withthis laser light. However, this laser light can be converted into ashorter wavelength by a non-linear optical element. Examples of harmonicthereof include the second harmonic (532 nm), the third harmonic (355nm), the fourth harmonic (266 nm), and the fifth harmonic (213 nm).These harmonics are absorbed in an amorphous silicon film at a highabsorption coefficient and therefore can be used in crystallization ofan amorphous silicon film.

In the above structure, the laser irradiation apparatus is characterizedin that the dividing means is one or more kinds selected from a slit, amirror, a prism, a cylindrical lens, and a cylindrical lens array.

In the above structure, the laser irradiation apparatus is characterizedin that the synthesizing means is one or more kinds selected from amirror and a cylindrical lens.

A structure of the present invention disclosed in this specification isa method of laser irradiation, characterized by comprising: dividingeach of plural first laser beams that are emitted from a plurality oflasers into plural second laser beams; choosing one laser beam out ofthe second laser beams for each of the plural first laser beams andsynthesizing the laser beams in the same region on an irradiationsurface or in the vicinity thereof.

In the above structure, the laser irradiation apparatus is characterizedin that the lasers are continuous wave or pulse oscillation solid-statelasers or gas lasers or metal lasers. Examples of the solid-state lasersinclude a continuous wave or pulse oscillation YAG laser, YVO₄ laser,YLF laser, YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandritelaser, and Ti:sapphire laser. Examples of the gas lasers include acontinuous wave or pulse oscillation excimer laser, Ar laser, Kr laser,and CO₂ laser. Examples of the metal lasers include a continuous wave orpulse oscillation helium cadmium laser, copper steam laser, and goldsteam laser.

In the above structure, the laser light is desirably converted intoharmonic by a non-linear optical element.

A structure of the present invention disclosed in this specification isa method of manufacturing a semiconductor device, characterized bycomprising: dividing each of plural first laser beams that are emittedfrom a plurality of lasers into plural second laser beams; choosing onelaser beam out of the second laser beams for each of the plural firstlaser beams to obtain third laser beams and synthesizing the third laserbeams in the same region on an irradiation surface or in the vicinitythereof to form a fourth laser beam; and irradiating a semiconductorfilm with the fourth laser beam while moving the laser beam relative tothe semiconductor film.

In the above structure, the laser irradiation apparatus is characterizedin that the lasers are continuous wave or pulse oscillation solid-statelasers or gas lasers or metal lasers. Examples of the solid-state lasersinclude a continuous wave or pulse oscillation YAG laser, YVO₄ laser,YLF laser, YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandritelaser, and Ti:sapphire laser. Examples of the gas lasers include acontinuous wave or pulse oscillation excimer laser, Ar laser, Kr laser,and CO₂ laser. Examples of the metal lasers include a continuous wave orpulse oscillation helium cadmium laser, copper steam laser, and goldsteam laser.

In the above structure, the laser light is desirably converted intoharmonic by a non-linear optical element.

In the above structure, the semiconductor film is desirably a filmcontaining silicon. A glass substrate, a quartz substrate, a siliconsubstrate, a plastic substrate, a metal substrate, a stainless steelsubstrate, a flexible substrate, etc. can be used as a substrate onwhich the semiconductor film is formed. Examples of the glass substrateinclude a barium borosilicate glass substrate and an aluminoborosilicateglass substrate. A flexible substrate means a substrate in the form of aPET, PES, PEN, or acrylic film or other similar film. When a flexiblesubstrate is used to manufacture a semiconductor device, the device canhave a reduced weight. It is desirable to form on the front side, or onthe front side and back side, of a flexible substrate a single layer ormulti-layer of aluminum films (AlON, AlN, AlO, or the like), carbonfilms (DLC (diamond-like carbon) or the like), or SiN films as a barrierlayer because the barrier layer improves the durability and otherproperties.

The present invention synthesizes laser beams emitted from differentlasers on an irradiation surface or in the vicinity thereof andtherefore interference does not take place. Most desirably, laser beamshaving different energy distributions from one another are synthesizedon an irradiation surface or in the vicinity thereof. However, since theoptimum synthesizing method varies from one laser light mode to another,the synthesizing method used can be chosen to suit individual cases. Forexample, laser light in the TEM_(oo) mode is highly symmetrical andtherefore laser light having a relatively high uniformity can beobtained by dividing laser light into two and synthesizing the left halfand right half thereof. Needless to say, more highly uniform laser lightis obtained when the number of division is larger. Laser light in othermodes can also provide highly uniform laser light using the same method.

The present invention can irradiate a semiconductor film formed on asubstrate with a rectangular beam having highly uniform energydistribution. Accordingly, a semiconductor film of uniform physicalproperty can be obtained. This makes it possible to reduce fluctuationin electric characteristic of TFTs manufactured from this semiconductorfilm. This also improves the operation characteristic and reliability ofa semiconductor device manufactured from these TFTs.

BRIEF DESCRIPTION OF THE DRAWINGS

In the accompanying drawings:

FIG. 1 is a diagram showing an example of an optical system of thepresent invention;

FIGS. 2A to 2C are diagrams showing an example of laser light beingdivided by the optical system of FIG. 1;

FIG. 3 is a diagram showing an example of an optical system of thepresent invention;

FIGS. 4A to 4E are diagrams showing an example of laser light beingdivided by the optical system of FIG. 3;

FIG. 5 is a diagram showing an example of a rectangular beam shapeformed on an irradiation surface by the optical system of FIG. 3;

FIG. 6 is a diagram showing an example of an optical system of thepresent invention;

FIG. 7 is a diagram showing an example of an optical system of thepresent invention;

FIG. 8 is a diagram showing an example of an optical system of thepresent invention;

FIG. 9 is a diagram showing an example of an optical system of thepresent invention;

FIG. 10 is a diagram showing an example of a conventional opticalsystem;

FIGS. 11A and 11B are a diagram showing an example of energy densitydistribution of laser light formed by a conventional optical system anda diagram showing an example of annealing a large-area substrate withthe laser light shown in FIG. 11A, respectively;

FIGS. 12A to 12C are sectional views showing a process of manufacturinga pixel TFT and TFTs of a driving circuit;

FIGS. 13A to 13C are sectional views showing a process of manufacturinga pixel TFT and TFTs of a driving circuit;

FIG. 14 is a sectional view showing a process of manufacturing a pixelTFT and TFTs of a driving circuit;

FIG. 15 is a top view showing the structure of a pixel TFT;

FIG. 16 is a sectional view of an active matrix liquid crystal displaydevice;

FIG. 17 is a sectional structural view of a driving circuit and pixelportion of a light emitting device;

FIGS. 18A to 18F are diagrams showing examples of a semiconductordevice;

FIGS. 19A to 19D are diagrams showing examples of a semiconductordevice;

FIGS. 20A to 20C are diagrams showing examples of a semiconductordevice;

FIG. 21 is a diagram showing an example of an optical system of thepresent invention;

FIGS. 22A to 22D are diagrams showing an example of laser light beingdivided by the optical system of FIG. 21;

FIG. 23 is a diagram for obtaining an incident angle θ of laser lightentering an irradiation object;

FIG. 24 is a diagram showing an example of an optical system of thepresent invention; and

FIG. 25 is a diagram showing an example of a laser light shape formed onan irradiation surface by the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Embodiment Mode 1

This embodiment mode describes with reference to FIG. 1 and FIGS. 2A to2C an example of optical system for dividing laser beams that areemitted from a plurality of lasers and overlapping laser beams that havedifferent energy distributions from one another.

A laser 101 a and a laser 101 b each emit laser light. The lasers 101 aand 101 b used here are continuous wave or pulse oscillation solid-statelasers, gas lasers, or metal lasers. Examples of the solid-state lasersinclude a continuous wave or pulse oscillation YAG laser, YVO₄ laser,YLF laser, YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandritelaser, and Ti:sapphire laser. Examples of the gas lasers include acontinuous wave or pulse oscillation excimer laser, Ar laser, Kr laser,and CO₂ laser. Examples of the metal lasers include a continuous wave orpulse oscillation helium cadmium laser, copper steam laser, and goldsteam laser. The laser light emitted from the lasers 101 a and 101 b maybe converted into harmonic by a non-linear optical element.

Denoted by 102 a and 102 b are isolators. If laser light used has highreflectance against an irradiation object and the laser light enters theirradiation object perpendicular to the object, the light goes back thelight path it used upon entering the irradiation object (return light).Return light affects laser apparatus by changing the laser output andfrequency and by breaking a rod. Components of the optical system inthis embodiment mode are arranged symmetrically and therefore reflectedlight of the two lasers on the irradiation surface may mutually affectthe other laser in a way similar to return light. This is why installingthe isolators 102 a and 102 b is desirable.

Each of the laser light emitted is expanded by beam expanders 103 a and104 a, or 103 b and 104 b. Beam expanders are effective especially whenlaser light emitted from a laser has a small shape, and may be omitteddepending on the size of laser light. The laser light may be expandednot only in one direction but also in two directions. The cylindricallenses 103 a, 104 a, 103 b, and 104 b are desirably made of syntheticsilica glass because it gives them high transmittance. Coating on thesurfaces of the cylindrical lenses 103 a and 104 a, or 103 b and 104 bis desirably capable of providing 99% or higher transmittance for thewavelength of laser light used.

The laser light that exits the beam expanders 103 a and 104 a or 103 band 104 b is divided in two directions by a mirror 105 a or 105 b. Themirror 105 a or 105 b dividing the laser light is described referring toFIGS. 2A and 2B. FIGS. 2A and 2B show laser light shapes in sectionperpendicular to the direction the laser light travels. Laser lightemitted from the laser 101 a is divided into first laser light andsecond laser light by the mirror 105 a as shown in FIG. 2A. The secondlaser light enters an irradiation object 108 whereas the first laserlight is absorbed by a damper 107 a. On the other hand, laser lightemitted from the laser 101 b is divided into third laser light andfourth laser light by the mirror 105 b as shown in FIG. 2B. The thirdlaser light enters the irradiation object 108 whereas the fourth laserlight is absorbed in a damper 107 b.

The two laser beams entering the irradiation object 108 do not interfereeach other even when synthesized because they are emitted from differentlasers. Since the second laser light of laser light emitted from thelaser 101 a enters the irradiation object and the third laser light oflaser light emitted from the laser 101 b enters the irradiation object,laser beams having different energy distributions are synthesized on theirradiation surface or in the vicinity thereof. As a result, rectangularlaser light having excellent uniformity in energy distribution isformed. (FIG. 2C)

The irradiation object 108 is irradiated with the thus formed laserlight while moving the laser light relative to the irradiation object108 in the direction indicated by 110 or 111, for example. This way adesired region of the irradiation object 108, or the entire regionthereof can be irradiated.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

In this embodiment mode, laser light is divided by a mirror but thepresent invention is not limited thereto. A slit, a prism, a cylindricallens, or a cylindrical lens array may be employed instead.

Although this embodiment mode uses two lasers and each laser light isdivided in two, the present invention is not limited thereto. Preferablyten or so lasers are used. When using a small number of lasers, it isdesirable to set the number of lasers to an even number and divide eachlaser light in an even number. Not all of lasers used may be identical.

In this embodiment mode, laser light is divided into equal widths by aplane perpendicular to the direction the laser light travels as shown inFIGS. 2A to 2C. However, the present invention is not limited thereto.

In this embodiment mode, laser beams having different energydistributions from one another are synthesized on an irradiation surfaceor in the vicinity thereof. However, since the optimum synthesizingmethod varies from one laser light mode to another, the synthesizingmethod used can be chosen to suit individual cases. For example, laserlight in the TEM_(oo) mode is highly symmetrical and therefore laserlight having a relatively high uniformity can be obtained by dividinglaser light into two and synthesizing the left half and right halfthereof. Needless to say, more highly uniform laser light is obtainedwhen the number of division is larger. Laser light in other modes canalso provide highly uniform laser light using the same method.

If the coating on the surface of synthesized silica glass is changed tosuite the wavelength of laser light used, the present invention can beapplied to various lasers.

Although a rectangular beam is formed in this embodiment mode so thatlaser light has a rectangular shape on an irradiation surface, the laserlight shape formed is not limited thereto. The laser light shape emittedfrom a laser is varied from one type of laser to another type and, evenwhen shaped by an optical system, the resultant shape tends to beinfluenced by the initial shape. For example, the laser light shapeemitted from a XeCl excimer laser may be a 10 mm×30 mm (both arehalf-width in beam profile) rectangle, and laser light emitted from asolid-state laser has a circular shape if the rod shape is cylindricaland a rectangular shape if the rod shape is slab-like. The presentinvention can be applied to laser light of any shape without a problemas long as the laser light has an energy density sufficient forannealing of an irradiation object.

Embodiment Mode 2

This embodiment mode describes with reference to FIGS. 21 to 23 anexample of optical system for dividing laser beams that are emitted fromthree of lasers and overlapping laser beams that have different energydistributions from one another.

Lasers 101 a to 101 c each emit laser light. The lasers 101 a to 101 cused here are continuous wave or pulse oscillation solid-state lasers,gas lasers, or metal lasers. Examples of the solid-state lasers includea continuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser. Examples of the gas lasers include a continuous waveor pulse oscillation excimer laser, Ar laser, Kr laser, and CO₂ laser.Examples of the metal lasers include a continuous wave or pulseoscillation helium cadmium laser, copper steam laser, and gold steamlaser. The laser light emitted from the lasers 101 a to 101 c may beconverted into harmonic by a non-linear optical element.

Though not shown, laser beams emitted from the lasers 101 a to 101 cseparately may be expanded by beam expanders. Beam expanders areeffective especially when laser light emitted from a laser has a smallshape.

Laser beams emitted from the lasers 101 a to 101 c are divided byoptical systems 102 a to 102 c, respectively, in two directions. Each ofthe optical systems 102 a to 102 c is a combination of a mirror and acylindrical lens. The optical systems 102 a to 102 c dividing the laserlight are shown in FIGS. 22A to 22D. Laser light emitted from the laser101 a is divided into three by the optical system 102 a and only theleft hand laser light of the three (first laser light in FIG. 22A)travels straight whereas the other two are reflected by the mirror andreach a damper 110 a. Laser light emitted from the laser 101 b isdivided into three by the optical system 102 b and only the center laserlight of the three (second laser light in FIG. 22B) travels straightwhereas the other two are reflected by the mirror and reach a damper 110b. Laser light emitted from the laser 101 c is divided into three by theoptical system 102 c and only the right hand laser light of the three(third laser light in FIG. 22C) travels straight whereas the other twoare reflected by the mirror and reach a damper 110 c. In this way theoptical systems 102 a to 102 c determine which laser light travelsstraight and which laser light is reflected.

Alternatively, each laser light may enter a cylindrical lens array to bedivided and then only a desired one out of divided laser beams may betaken out using a slit that has a reflective surface.

The laser beams traveling straight through the optical systems 102 a to102 c respectively pass through mirrors 103 a to 103 c and enter convexlenses 104 a to 104 c at angles. This causes aberration such asastigmatism to shift the focal point and make it possible to form arectangular beam 106 on an irradiation surface or in the vicinitythereof. As shown in FIGS. 22A to 22D, laser beams that have passedthrough the optical systems 102 a and 102 c are longitudinally shorterthan a laser beam that has passed the optical system 102 b. Thereforelaser beams that have passed through the optical systems 102 a and 102 care more slanted than a laser beam that has passed the optical system102 b when the beams enter the lenses. This makes them longer in thelongitudinal direction so that the three laser beams have the samelength in the longitudinal direction. Alternatively, the shorter twolaser beams may be expanded by a cylindrical lens or the like.

Coating on the surfaces of the convex lenses 104 a to 104 c is desirablycapable of providing 99% or higher transmittance for the wavelength oflaser light used. Furthermore, it is desirable to use as the convexlenses aspherical lenses in which spherical aberration is corrected.With the use of aspherical lenses, light collection is improved as wellas the aspect ratio and energy density distribution.

The laser beams that have passed through the convex lenses 104 a to 104c are synthesized on an irradiation surface or in the vicinity thereofto form a rectangular beam 106 (FIG. 22D). The thus formed rectangularbeam does not interfere since laser beams used to form the beam 106 areemitted from different lasers. In addition, the rectangular beam hasexcellent uniformity in energy distribution because plural laser beamshaving different energy distributions are synthesized on an irradiationsurface or in the vicinity thereof.

An irradiation object 105 is irradiated with the thus formed rectangularbeam while moving the beam relative to the irradiation object 105 in thedirection indicated by 108 or 109, for example. This way a desiredregion of the irradiation object 105, or the entire region thereof canbe irradiated.

However, depending on the wavelength of laser light, light reflected bythe surface of the irradiation object 105 may interfere with lightreflected by the back side of a substrate on which the irradiationobject 105 is formed. FIG. 23 shows an example in which a semiconductorfilm 11 is formed as the irradiation object 105 on a substrate 10. Iflight reflected by the semiconductor film 11 and light reflected by theback side of the substrate 10 do not overlap each other, interference ofthe reflected light does not take place.

In this case, when an incident face is defined as a plane which isperpendicular to the irradiation surface and which includes a shorterside or longer side of the rectangle shape of the long beam, an incidentangle θ of the laser light desirably satisfies θ≧arctan(W/2d), whereinthe length of the shorter side or longer side included in the incidentface is given as W and the thickness of a substrate transmissive of thelaser light is given as d. The symbol W in the expression satisfiesW=(w₁+w₂)/2 when w₁ represents a beam length 15 upon entering theirradiation object and w₂ represents the length of the beam reflected bythe back side of the substrate 10. If the laser light track is not onthe incident face, the track is projected onto the incident face and theincident angle thereof is set as θ. When laser light enters the incidentface at this incident angle θ, light reflected by the front side of thesubstrate and light reflected by the back side of the substrate do notinterfere each other and uniform laser light irradiation can beobtained. If the incident angle θ with respect to the irradiation objectis set to Brewster angle, the reflectance is reduced to the lowest leveland therefore laser light can be used efficiently. The above discussionis on the premise that the refractive index of the substrate is 1. Inpractice, the refractive index of most substrates is around 1.5 and, ifthe calculation is based on this value, the angle obtained is largerthan the one calculated in the above discussion. However, the energy ofa linear beam is attenuated at both edges in the longitudinal directionto lessen the influence of interference at the edges and therefore asatisfactory level of interference attenuation effect is obtained at thecalculated value of the above discussion. Desirably, the incident angleof every laser light that enters the irradiation surface satisfies theabove expression, θ≧arctan(W/2d).

A reflection preventive film may be formed on the surface of anirradiation object.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Although this embodiment mode uses three lasers and each laser light isdivided in three, the present invention is not limited thereto.

In this embodiment mode, laser light is divided into equal widths by aplane perpendicular to the direction the laser light travels as shown inFIG. 22. However, the present invention is not limited thereto.

The laser light shape emitted from a laser is varied from one type oflaser to another type and, even when shaped by an optical system, theresultant shape tends to be influenced by the initial shape. Forexample, the laser light shape emitted from a XeCl excimer laser isrectangular, and laser light emitted from a solid-state laser has acircular shape if the rod shape is cylindrical and a rectangular shapeif the rod shape is slab-like. The present invention can be applied tolaser light of any shape.

More detailed description will be given on the present inventionstructured as above using the following embodiments.

Embodiment 1

This embodiment describes with reference to FIG. 3 and FIGS. 4A to 4E anexample of optical system for dividing laser beams that are emitted fromfour lasers and overlapping laser beams that have different energydistributions from one another.

Lasers 131 a to 131 d each emit laser light. The lasers 131 a to 131 dused here are continuous wave or pulse oscillation solid-state lasers,gas lasers, or metal lasers. Examples of the solid-state lasers includea continuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser. Examples of the gas lasers include a continuous waveor pulse oscillation excimer laser, Ar laser, Kr laser, and CO₂ laser.Examples of the metal lasers include a continuous wave or pulseoscillation helium cadmium laser, copper steam laser, and gold steamlaser. The laser light emitted from the lasers 131 a to 131 d may beconverted into harmonic by a non-linear optical element.

In this embodiment, a continuous wave YVO₄ laser is used and its laserlight is converted into the second harmonic by a non-linear opticalelement. The beam diameter of the laser light is 2.25 mm and the beamspread angle is set to 0.35 mrad.

Though not shown in the drawing, it is desirable to install isolators.This is because components of the optical system in this embodiment arearranged symmetrically and therefore reflected light of lasers on anirradiation surface may mutually affect other lasers in a way similar toreturn light.

Beam expanders (not shown) may be provided to expand laser light in thelongitudinal direction and lateral direction. Beam expanders areeffective especially when laser light emitted from a laser has a smallshape.

Laser beams emitted from the lasers 131 a to 131 d are divided by slits132 a to 132 d having reflective surfaces, respectively, so that eachlaser light is divided in two directions. Positioning of a slit withrespect to laser light is varied among the slits 132 a to 132 d, andwhich one of divided laser beams travels straight varies from one slitto another. The laser beams being divided by the slits are describedreferring to FIGS. 4A to 4D. FIGS. 4A to 4D each show a laser lightshape in section perpendicular to the direction the laser light travels.FIG. 4A shows laser light emitted from the laser 131 a. The laser lightis divided by the slit 132 a into four, and a first laser beam travelsstraight whereas second to fourth laser beams are reflected and absorbedin a damper 137. FIG. 4B shows laser light emitted from the laser 131 b.The laser light is divided by the slit 132 b into four, and a secondlaser beam travels straight whereas first, third, and fourth laser beamsare reflected and absorbed in the damper 137. FIG. 4C shows laser lightemitted from the laser 131 c. The laser light is divided by the slit 132c into four, and a third laser beam travels straight whereas first,second, and fourth laser beams are reflected and absorbed in the damper137. FIG. 4D shows laser light emitted from the laser 131 d. The laserlight is divided by the slit 132 d into four, and a fourth laser beamtravels straight whereas first to third laser beams are reflected andabsorbed in the damper 137. As described, each of the slits 132 a to 132d lets one laser beam out of divided laser beams to travel straightwhereas the rest of the divided laser beams are reflected, and a laserbeam allowed to travel straight by one slit has different energydistribution than a laser beam allowed to travel straight by anotherslit.

The travel directions of the laser beams that have passed through theslits 132 a to 132 d are changed by prisms 133 a to 133 d, respectively.The prisms 133 a to 133 d are provided to synthesize all of the fourlaser beams at the same irradiation position.

If laser light that reaches the irradiation surface is one at an edge ofthe initial laser light, it is desirable to expand the length of thislaser light in the longitudinal direction by a cylindrical lens 134 a or134 d. As shown in FIGS. 4A to 4D, the length of laser light is shorterat its edges than around the center. Therefore, if the lengths of laserlight edges are adjusted to have the same length as the center of thelaser light prior to synthesization on the irradiation surface or in thevicinity thereof, a rectangular beam of high uniformity can be obtainedupon the synthesization. In this embodiment, cylindrical lenses eachhaving a focal length of 50 mm are placed such that the curvature isparallel to the longitudinal direction.

The laser beams are synthesized as shown in FIG. 4E on the irradiationsurface by the optical system structured as above. The shape of laserlight formed on the irradiation surface is simulated and the resultthereof is shown in FIG. 5. FIG. 5 shows that a rectangular beam 7.1 mmin width and 22.2 mm in length is obtained. Since the laser beams usedto form this rectangular beam are emitted from different lasers,interference does not take place. In addition, the rectangular beam hasexcellent uniformity in energy distribution because plural laser beamshaving different energy distributions are synthesized on the irradiationsurface.

An irradiation object 108 is irradiated with the thus formed rectangularbeam while moving the beam relative to the irradiation object 108 in thedirection indicated by 110 or 111, for example. This way a desiredregion of the irradiation object 108, or the entire region thereof canbe irradiated.

Although this embodiment uses four lasers and each laser light isdivided into four, the present invention is not limited thereto.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Embodiment 2

This embodiment describes with reference to FIG. 6 an example of opticalsystem for dividing laser beams that are emitted from three lasers andoverlapping laser beams that have different energy distributions fromone another.

Lasers 121 a to 121 c each emit laser light. The lasers 121 a to 121 cused here are continuous wave or pulse oscillation solid-state lasers,gas lasers, or metal lasers. Examples of the solid-state lasers includea continuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser. Examples of the gas lasers include a continuous waveor pulse oscillation excimer laser, Ar laser, Kr laser, and CO₂ laser.Examples of the metal lasers include a continuous wave or pulseoscillation helium cadmium laser, copper steam laser, and gold steamlaser. The laser light emitted from the lasers 121 a to 121 c may beconverted into harmonic by a non-linear optical element.

In this embodiment, a pulse oscillation YAG laser is used and its laserlight is converted into the second harmonic by a non-linear opticalelement.

The laser beams emitted are separately expanded by beam expanders 122 ato 122 c and then by beam expanders 123 a to 123 c. Beam expanders areeffective especially when laser light emitted from a laser has a smallshape, and may be omitted depending on the size of laser light. Thecylindrical lenses 122 a to 122 c and 123 a to 123 c are desirably madeof synthetic silica glass because it gives them high transmittance.Coating on the surfaces of the cylindrical lenses 122 a to 122 c and 123a to 123 c is desirably capable of providing 99% or higher transmittancefor the wavelength of laser light used.

The laser beams that exit the beam expanders 122 a to 122 c and 123 a to123 c are respectively divided in two directions by optical systems 124a to 124 c. Each of the optical systems 124 a to 124 c is a combinationof a mirror and a cylindrical lens. Laser light emitted from the laser121 a is divided into three by the optical system 124 a, and only theleft laser light of the three travels straight whereas the other two arereflected by the mirror and reach a damper 126. Laser light emitted fromthe laser 121 b is divided into three by the optical system 124 b andonly the center laser light of the three travels straight whereas theother two are reflected by the mirror and reach the damper 126. Laserlight emitted from the laser 121 c is divided into three by the opticalsystem 124 c and only the right laser light of the three travelsstraight whereas the other two are reflected by the mirror and reach thedamper 126. In this way the optical systems 124 a to 124 c determinewhich laser light travels straight and which laser light is reflected.

Alternatively, each laser light may enter a cylindrical lens array to bedivided and then only a desired one out of divided laser light may betaken out using a slit that has a reflective surface.

If laser light that reaches the irradiation surface is one at an edge ofthe initial laser light, it is desirable to expand the length of thislaser light in the longitudinal direction by a cylindrical lens or thelike (not shown) because edges of laser light are shorter in length thanthe center of the laser light.

The laser beams that have passed through the optical systems 124 a to124 c are synthesized by a cylindrical lens 125 on the irradiationsurface or in the vicinity thereof to form a rectangular beam. The thusformed rectangular beam does not interfere since laser beams used toform the rectangular beam are emitted from different lasers. Inaddition, the rectangular beam has excellent uniformity in energydistribution because plural laser beams having different energydistributions are synthesized on the irradiation surface or the vicinitythereof.

An irradiation object 108 is irradiated with the thus formed rectangularbeam while moving the beam relative to the irradiation object 108 in thedirection indicated by 110 or 111, for example. This way a desiredregion of the irradiation object 108, or the entire region thereof canbe irradiated.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Although this embodiment uses three lasers and the laser light isdivided into three, the present invention is not limited thereto.

This embodiment may be combined freely with Embodiment 1.

Embodiment 3

In this Embodiment, an optical system example of forming simultaneouslya plurality of laser beams will be described by using the FIG. 7 thatlaser beams which are oscillated from two lasers are divided and laserbeams whose energy densities are different from each other areoverlapped.

Laser beams are respectively irradiated from laser 141 a and laser 141b. Here, a solid state laser, a gas laser, or a metal laser of acontinuous oscillation or a pulse oscillation are used as lasers 141 aand 141 b.

It should be noted that as the above-mentioned solid state laser, YAGlaser, YVO₄ laser, YLF laser, YAlO₃ laser, Y₂O₃ laser, glass laser, rubylaser, alexandrite laser, Ti: sapphire laser or the like of continuousoscillation or pulse oscillation are listed, as the above-mentioned gaslaser, excimer laser, Ar laser, Kr laser, CO₂ laser or the like ofcontinuous oscillation or pulse oscillation are listed, and as theabove-mentioned metal laser, helium-cadmium laser, copper vapor laser,gold vapor laser and the like are listed. Further, laser beamsirradiated from laser 141 a and laser 141 b may be converted into thehigher harmonic wave by a non-linear optical element.

In this embodiment, lasers 141 a and 141 b are converted into the thirdhigher harmonic wave by a continuous oscillation YAG lasers

Irradiated laser beams are expanded by beam expanders 142 a and 143 a or142 b and 143 b. It should be noted that a beam expander is particularlyeffective in case, shapes of laser beams irradiated from lasers aresmall so that a beam expander is not used necessarily according to thesize and the like of laser beams. It is desirable to obtain a hightransmittance if a cylindrical lenses 142 a, 143 a, 142 b, 143 b aremade of synthetic quartz glass. It is also desirable that coatings givento surfaces of lenses 142 a, 143 a, 142 b and 143 b can be obtained morethan 99% transmittance against the wave length of the laser beam whichis used.

Laser beam irradiated from beam expanders 142 and 143 are divided intotwo directions by the optical systems 144 a and 144 b combined mirrorsand cylindrical lenses. Right laser beam of division into two whichoscillated from the laser 141 a by the optical system 144 a goesstraight and left laser beam reflects with the mirror. Left laser beamof division into two which oscillated from the laser 141 b by theoptical system 144 b goes straight and right laser beam reflects withthe mirror. In this way, laser beam are determined to go straight or toreflect by optical systems 144 a and 144 b.

Laser beams which go straight by optical systems 144 a and 144 b aresynthesized at the irradiation side or near it by the cylindrical lens147 a and forms rectangular shape beams. Rectangular shape beams whichformed in this way are not interfered because they are oscillated bydifferent lasers. Rectangular shape beams with excellent uniformity ofenergy densities are formed because a plurality of laser beams withdifferent energy densities are formed at the irradiation side or nearit.

While, laser beams which reflect by optical systems 144 a and 144 b aresynthesized at the irradiation side or near it by the cylindrical lenses146 a, 146 b and 147 b and form rectangular shape beams. Rectangularshape beams which formed in this way are not interfered because they areoscillated by different lasers. Rectangular shape beams with excellentuniformity of energy densities are formed because a plurality of laserbeams with different energy densities are formed at the irradiation sideor near it.

Then, while a plurality of rectangular shape beams formed in this wayirradiate, they can irradiate the desired region or whole area on theirradiated body 108 by being relatively moved with respect to theirradiated body 108, for example, in the direction indicated with thereference numerals 110 and 111. Moreover, the through-put can beimproved because a plurality of rectangular shape beams are formed.

The semiconductor film can be crystallized, a crystalline semiconductorfilm can be obtained with improving the crystalline and the activationof the impurity element can be performed if a semiconductor film isannealed by using such a laser irradiation apparatus

It should be noted that in this embodiment, although an example in whichtwo lasers are used and the division number of laser beams is two, it isnot limited and the number of rectangular shape beams which are formedare not limited two.

This embodiment can be combined with Embodiments 1 or 2 freely.

Embodiment 4

This embodiment describes with reference to FIG. 8 an example of opticalsystem for dividing laser beams that are emitted from four lasers andoverlapping laser beams that have different energy distributions fromone another.

Lasers 151 a to 151 d each emit laser light. The lasers 151 a to 151 dused here are continuous wave or pulse oscillation solid-state lasers,gas lasers, or metal lasers. Examples of the solid-state lasers includea continuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser. Examples of the gas lasers include a continuous waveor pulse oscillation excimer laser, Ar laser, Kr laser, and CO₂ laser.Examples of the metal lasers include a continuous wave or pulseoscillation helium cadmium laser, copper steam laser, and gold steamlaser. The laser light emitted from the lasers 151 a to 151 d may beconverted into harmonic by a non-linear optical element.

In this embodiment, a pulse oscillation YAG laser is used and its laserlight is converted into the second harmonic by a non-linear opticalelement. The second harmonic of a YAG laser can be transmitted through aglass substrate or a quartz substrate and therefore is preferable when asubstrate is irradiated from both sides as in this embodiment.

The laser beams emitted are separately expanded by beam expanders 152 ato 152 d and then by beam expanders 153 a to 153 d. Beam expanders areeffective especially when laser light emitted from a laser has a smallshape, and may be omitted depending on the size of laser light. Thecylindrical lenses 152 a to 152 d and 153 a to 153 d are desirably madeof synthetic silica glass because it gives them high transmittance.Coating on the surfaces of the cylindrical lenses 152 a to 152 d and 153a to 153 d is desirably capable of providing 99% or higher transmittancefor the wavelength of laser light used.

The laser beams that exit the beam expanders 152 a to 152 d and 153 a to153 d are respectively divided in two directions by optical systems 154a to 154 d. Each of the optical systems 154 a to 154 d is a combinationof a mirror and a cylindrical lens. Laser light emitted from the laser151 a is divided into four by the optical system 154 a, and only themost left laser light of the four travels straight whereas the other twoare reflected by the mirror and reach a damper 156 a. Laser lightemitted from the laser 151 b is divided into four by the optical system154 b and only the second left laser light of the four travels straightwhereas the other regions are reflected by the mirror and reach thedamper 156 a. Laser light emitted from the laser 151 c is divided intofour by the optical system 154 c and only the second right laser lightof the four travels straight whereas the other three are reflected bythe mirror and reach the damper 156 c. Laser light emitted from thelaser 151 d is divided into four by the optical system 154 s and onlythe most right laser light of the four travels straight whereas theother three are reflected by the mirror and reach the damper 156 c. Inthis way the optical systems 154 a to 154 d determine which laser lighttravels straight and which laser light is reflected.

Alternatively, each laser light may enter a cylindrical lens array to bedivided and then only a desired one out of divided laser beams may betaken out using a slit that has a reflective surface.

Though not shown, laser light at an edge of the divided regions isdesirably expanded by a cylindrical lens array or the like since laserlight at an edge is shorter in the longitudinal direction than laserlight near the center.

The laser beams that have passed through the optical systems 154 a to154 d are synthesized by cylindrical lenses 155 a and 155 c on theirradiation surface or in the vicinity thereof to form a rectangularbeam. The thus formed rectangular beam does not interfere since laserbeams used to form the rectangular beam are emitted from differentlasers. In addition, the rectangular beam has excellent uniformity inenergy distribution because plural laser beams having different energydistributions are synthesized on the irradiation surface or the vicinitythereof.

An irradiation object 108 is irradiated with the thus formed rectangularbeam while moving the beam relative to the irradiation object 108 in thedirection indicated by 110 or 111, for example. This way a desiredregion of the irradiation object 108, or the entire region thereof canbe irradiated.

When plural laser beams irradiate one side of the substrate and aresynthesized at the same irradiation position, the laser beams havedifferent light path lengths and spread angles of the laser beams mayexpand the synthesized beam unnecessarily, thereby lowering uniformityin energy distribution. The structure of this embodiment is free fromthis problem because the plural laser beams each have the same lightpath length to reach the irradiation surface.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Although this embodiment uses four lasers and each laser light isdivided into four, the present invention is not limited thereto.

This embodiment may be combined freely with Embodiments 1 to 3.

Embodiment 5

This embodiment gives a description with reference to FIG. 9 an exampleof optical system for dividing laser beams that are emitted from fourlasers, overlapping and synthesizing laser beams that have differentenergy distributions, and irradiating a substrate from both sides.

In FIG. 9, an optical system is composed of lasers 101 a and 101 b,isolators 102 a and 102 b, beam expanders 103 a and 104 a or 103 b and104 b, mirrors 105 a and 105 b, mirrors 106 a and 106 b, an irradiationobject 108, and a stage 109. The optical system is similar to thestructure shown in Embodiment Mode 1 (FIG. 1).

In this embodiment, a YLF laser is used and its laser light is convertedinto the second harmonic. The second harmonic of a YLF laser can betransmitted through a glass substrate or a quartz substrate andtherefore is preferable when a substrate is irradiated from both sidesas in this embodiment. Even when the laser has a wavelength that doesnot allow a substrate to transmit it, the substrate can be partiallyannealed and it can be used in this embodiment.

Another optical system has the structure of FIG. 1 and is composed oflasers 101 c and 101 d, isolators 102 c and 102 d, beam expanders 103 cand 104 c or 103 d and 104 d, mirrors 105 c and 105 d, and mirrors 106 cand 106 d. This optical system and the above optical system are arrangedsuch that they are symmetrical with respect to the irradiation object108.

With this structure, the substrate can be irradiated with rectangularbeams from both sides. The irradiation object 108 is irradiated with thethus formed rectangular beams while moving the beams relative to theirradiation object 108 in the direction indicated by 110 or 111, forexample. This way a desired region of the irradiation object 108, or theentire region thereof can be irradiated.

By irradiating the substrate from both sides, the energy density can beenhanced. When plural laser beams irradiate one side of the substrateand are synthesized at the same irradiation position, the laser beamseach have different light path lengths and spread angles of the laserbeams may expand the synthesized beam unnecessarily, thereby loweringuniformity in energy distribution. The structure of this embodiment isfree from this problem because the plural laser beams each have the samelight path length to reach the irradiation surface.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Although this embodiment uses four lasers and each laser light isdivided into two, the present invention is not limited thereto.

This embodiment may be combined freely with Embodiments 1 to 4.

Embodiment 6

This embodiment describes with reference to FIGS. 4A to 4E, 24, and 25an example of optical system for dividing laser beams that are emittedfrom four lasers and overlapping laser beams that have different energydistributions from one another.

Lasers 131 a to 131 d each emit laser light. The lasers 131 a to 131 dused here are continuous wave or pulse oscillation solid-state lasers,gas lasers, or metal lasers. Examples of the solid-state lasers includea continuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser. Examples of the gas lasers include a continuous waveor pulse oscillation excimer laser, Ar laser, Kr laser, and CO₂ laser.Examples of the metal lasers include a continuous wave or pulseoscillation helium cadmium laser, copper steam laser, and gold steamlaser. The laser light emitted from the lasers 131 a to 131 d may beconverted into harmonic by a non-linear optical element.

In this embodiment, a continuous wave YVO₄ laser is used and its laserlight is converted into the second harmonic by a non-linear opticalelement. The beam diameter of the laser light is 2.25 mm and the beamspread angle is set to 0.35 mrad.

Though not shown in the drawing, it is desirable to install isolators.This is because components of the optical system in this embodiment arearranged symmetrically and therefore reflected light of lasers on anirradiation surface may mutually affect other lasers in a way similar toreturn light.

Beam expanders (not shown) may be provided to expand laser light in thelongitudinal direction and lateral direction. Beam expanders areeffective especially when laser light emitted from a laser has a smallshape.

Laser beams emitted from the lasers 131 a to 131 d are divided by slits132 a to 132 d having reflective surfaces, respectively, so that eachlaser light is divided in two directions. Positioning of a slit withrespect to laser light is varied among the slits 132 a to 132 d, andwhich one of divided laser beams travels straight varies from one slitto another. The laser beams being divided by the slits are describedreferring to FIGS. 4A to 4D. FIGS. 4A to 4D each show a laser lightshape in section perpendicular to the direction the laser light travels.FIG. 4A shows laser light emitted from the laser 131 a. The laser lightis divided by the slit 132 a into four, and a first laser beam travelsstraight whereas second to fourth laser beams are reflected and absorbedin a damper 135 a. FIG. 4B shows laser light emitted from the laser 131b. The laser light is divided by the slit 132 b into four, and a secondlaser beam travels straight whereas first, third, and fourth laser beamsare reflected and absorbed in the damper 135 a. FIG. 4C shows laserlight emitted from the laser 131 c. The laser light is divided by theslit 132 c into four, and a third laser beam travels straight whereasfirst, second, and fourth laser beams are reflected and absorbed in thedamper 135 c. FIG. 4D shows laser light emitted from the laser 131 d.The laser light is divided by the slit 132 d into four, and a fourthlaser beam travels straight whereas first to third laser beams arereflected and absorbed in the damper 135 c. As described, each of theslits 132 a to 132 d lets one laser beam out of divided laser beams totravel straight whereas the rest of the divided laser beams arereflected, and a laser beam allowed to travel straight by one slit hasdifferent energy distribution than a laser beam allowed to travelstraight by another slit.

Laser beams that have passed through the slits 132 a to 132 d enterconvex lenses 134 a to 134 d 4, respectively, at angles. This causesaberration such as astigmatism to shift the focal point and make itpossible to form a rectangular beam 106 on an irradiation surface or inthe vicinity thereof. In this embodiment, the radius of curvature of theconvex lenses 134 a and 134 d is set to 7 mm and the radius of curvatureof the convex lenses 134 b and 134 c is set to 9 mm. As shown in FIGS.4A to 4D, the length of laser light is shorter at edges than around thecenter. Therefore, by giving different radii of curvature, laser lightat an edge of initial laser light is expanded in length in thelongitudinal direction more than laser light at the center of theinitial laser light is expanded. This way a rectangular beam of highuniformity can be obtained upon synthesization on the irradiationsurface or in the vicinity thereof. Alternatively, a cylindrical lens orthe like may be used to expand laser light in the longitudinal directionif the laser light that reaches the irradiation surface is one at anedge of the initial laser light.

The shape of laser light formed on the irradiation surface by theoptical system structured as above is shown in FIG. 4E. The shape oflaser light formed on the irradiation surface is simulated and theresult thereof is shown in FIG. 25. FIG. 25 shows that a rectangularbeam 190 μm in width and 950 μm in length is obtained. Since the laserbeams used to form this rectangular beam are emitted from differentlasers, interference does not take place. In addition, the rectangularbeam has excellent uniformity in energy distribution because plurallaser beams having different energy distributions are synthesized on theirradiation surface.

An irradiation object 105 is irradiated with the thus formed rectangularbeam while moving the beam relative to the irradiation object 105 in thedirection indicated by 108 or 109, for example. This way a desiredregion of the irradiation object 105, or the entire region thereof canbe irradiated.

Although this embodiment uses four lasers and each laser light isdivided into four, the present invention is not limited thereto.

If this laser irradiation apparatus is used to anneal a semiconductorfilm, the semiconductor film can be crystallized, the crystallinity isimproved to obtain a crystalline semiconductor film, and an impurityelement can be activated.

Embodiment 7

A method of manufacturing an active matrix substrate is explained inthis embodiment using FIGS. 12 to 15. A substrate on which a CMOScircuit, a driver circuit, and a pixel portion having a TFT pixel and aholding capacity are formed together is called active matrix substratefor convenience.

First, a substrate 400 made from glass such as barium borosilicate glassor aluminum borosilicate glass is used in this embodiment. Note thatsubstrates such as quartz substrates, silicon substrates, metallicsubstrates, and stainless steel substrates having an insulating filmformed on the substrate surface may also be used as the substrate 400.Further, a plastic substrate having heat resisting properties capable ofenduring the processing temperatures used in this embodiment may also beused. Because this invention can form a plurality of rectangular shapebeams with a uniform energy distribution, it is possible that annealingthe large area substrate is conducted effectively by using a pluralityof rectangular shape beams.

Next, a base film 401 made from an insulating film such as a siliconoxide film, a silicon nitride film, or a silicon oxynitride film is thenformed on the substrate 400 by the known method. A two layer structureis used as the base film 401 in this embodiment, but a single layer ofthe above-mentioned insulating film may also be used, and a structure inwhich more than two layers are laminated may also be used.

Next, semiconductor layers are formed on the base film. First of all,semiconductor film is formed with a thickness of 25 to 200 nm(preferably 30 to 150 nm) by a known method (such as the sputteringmethod, the LPCVD method, and the plasma CVD method). Then, thesemiconductor film is crystallized by a laser crystallization method. Asthe laser crystallization method, the laser beam irradiates to thesemiconductor film by applying one of Embodiments 1 to 6 or by freelycombining any one of Embodiments 1 to 6. It is desirable that asolid-state laser of continuous oscillation or pulse oscillation, a gaslaser, or metallic laser is used. Note that, as the above-mentionedsolid-state laser, there may be given a YAG laser of a continuousoscillation or pulse oscillation, a YVO₄ laser, a YLF laser, a YAlO₃laser, Y₂O₃ laser, a glass laser, a ruby laser, an alexandrite laser, aTi:sapphire laser, and the like. As the above-mentioned gas laser, theremay be given a excimer laser of continuous oscillation or pulseoscillation, Ar laser, Kr laser, CO₂ laser, or the like. And as theabove-mentioned metallic laser, there may be given a helium cadmiumlaser, a copper vapor laser, or a gold vapor laser. Of course, not onlythe laser crystallization method but also any other knowncrystallization method (RTA, the thermal crystallization method using afurnace annealing, the thermal crystallization method using metallicelements which promote crystallization) may also be combined. Theabove-mentioned semiconductor film may be an amorphous semiconductorfilm, a microcrystal semiconductor film, a crystalline semiconductorfilm and the like. Alternatively, the semiconductor film may be acompound semiconductor film having an amorphous structure such as anamorphous silicon germanium film.

In this embodiment, plasma CVD method is used to form an amorphoussilicon film with a thickness of 50 nm, and then the thermalcrystallization method using metallic elements, which promotecrystallization, and laser crystallization method are used for theamorphous silicon film. Nickel is used as a metal element, and isintroduced onto the amorphous silicon film by a solution coating method.Then heat treatment is conducted at 550° C. for five hour, wherebyobtaining a first crystalline silicon film. Subsequently, the laser beamshot from a continuous oscillation YVO₄ laser with output 10 W isconverted into the second higher harmonic wave by a nonlinear opticalelement and then a rectangular shape beam is formed and irradiated byone of the optical system shown in Embodiments 1 thorough 6 or by theoptical system combined these embodiments, whereby obtaining a secondcrystalline silicon film. Irradiating the laser beam to the firstcrystalline silicon film, and changing the first crystalline siliconfilm to the second crystalline silicon film improve the crystallinity ofthe second crystalline silicon film. At this moment, about 0.01 to 100MW/cm² (preferably 0.1 to 10 MW/cm²) is necessary for the energydensity. The stage is relatively moved to the laser beam at a speed ofabout 0.5 to 2000 cm/s, and it irradiates, and then the crystallinesilicon film is formed. When the excimer laser of pulse oscillation isused, it is desirable that 300 Hz of frequency and 100 to 1000 mJ/cm²(typically, 200 to 800 MJ/cm²) of laser energy density are used. At thismoment, laser beam may be overlapped by 50 to 98%.

Of course, although a TFT can be formed by using the first crystallinesilicon film, it is desirable that the second crystalline silicon filmis used to form the TFT since the second crystalline silicon film has animproved crystallinity and electric characteristics of TFT are improved.For instance, although, when TFTs formed by using the first crystallinesilicon film, a mobility is almost 300 cm²/Vs, when TFT is formed byusing the second crystalline silicon film, the mobility is extremelyimproved with about 500 to 600 cm²/Vs.

The semiconductor layers 402 to 406 are formed by performing patterningprocessing on thus obtained semiconductor film by using thephotolithography method.

Doping of a very small amount of an impurity element (boron orphosphorous) may be performed after forming the semiconductor layers 402to 406 in order to control a TFT threshold value.

A gate insulating film 407 is formed next, covering the semiconductorlayers 402 to 406. The gate insulating film 407 is formed by aninsulating film containing silicon with a thickness of 40 to 150 nmusing plasma CVD or sputtering. In this embodiment, a silicon oxynitridefilm having a film thickness of 110 nm is formed by plasma CVD method.The gate insulating film is of course not limited to a siliconoxynitride film, and other insulating films containing silicon may beused in a single layer or in a lamination structure.

Further, if a silicon oxide film is used, it can be formed by plasma CVDmethod with a mixture of TEOS (Tetraethyl Orthosilicate) and O₂, at areaction pressure of 40 Pa, with the substrate temperature set from 300to 400° C., and by discharging at a high frequency (13.56 MHz) electricpower density of 0.5 to 0.8 W/cm². Good characteristics as a gateinsulating film can be obtained by subsequently performing thermalannealing, at between 400 and 500° C., of the silicon oxide film thusmanufactured.

A first conductive film 408 having a film thickness of 20 to 100 nm, anda second conductive film 409 having a film thickness of 100 to 400 nmare then formed and laminated on the gate insulating film 407. The firstconductive film 408, made from a TaN film having a film thickness of 30nm, and the second conductive film 409, made from a W film having a filmthickness of 370 nm, are formed and laminated in this embodiment. TheTaN film is formed by sputtering, and sputtering of a Ta target isperformed in a nitrogen atmosphere. Further, the W film is formed bysputtering using a W target. In addition, the W film can also be formedby thermal CVD method using tungsten hexafluoride (WF₆). Whichever isused, it is necessary to be able to make the film become low resistancein order to use it as a gate electrode, and it is desirable that theresistivity of the W film be made less than 20 μΩcm.

Note that although the first conductive film 408 is TaN and the secondconductive film 409 is W in this embodiment, there are no particularlimitations placed on the conductive films. The first conductive film408 and the second conductive film 409 may also be formed from anelement selected from the group consisting of Ta, W, Ti, Mo, Al, Cu, Cr,and Nd, or from an alloy material having one of these elements as itsmain constituent, or from a chemical compound of these elements.Further, a semiconductor film, typically a polycrystalline crystallinesilicon film, into which an impurity element such as phosphorous isdoped may also be used, as may an AgPdCu alloy.

Masks 410 to 415 are formed next from resist using a photolithographymethod, and a first etching process is performed in order to formelectrodes and wirings. The first etching processing is performed inaccordance with first and second etching conditions (FIG. 12B). An ICP(Inductively Coupled Plasma) etching method is used as a first etchingcondition in this embodiment. A gas mixture of CF₄, Cl₂, and O₂ is usedas an etching gas, the gas flow rates are set to 25:25:10 (sccm),respectively, a plasma is generated by supplying a 500 W RF (13.56 MHz)electric power to a coil shape electrode at a pressure of 1 Pa; andetching is performed. A 150 W RF (13.56 MHz) electric power is alsoapplied to the substrate side (sample stage), thereby applying asubstantially negative self-bias voltage. The W film is etched under thefirst etching conditions, and the edge portion of the first conductivelayer is made into a tapered shape.

The etching conditions are changed to a second etching condition withoutremoving the masks 410 to 415 made of resist. A gas mixture of CF₄ andCl₂ is used as an etching gas, the gas flow rates are set to 30:30(sccm), respectively, a plasma is generated by applying a 500 W RF(13.56 MHz) electric power to a coil shape electrode at a pressure of 1Pa, and etching is performed for approximately 30 seconds. A 20 W RF(13.56 MHz) electric power is also supplied to the substrate side(sample stage), thereby applying a substantially negative self-biasvoltage. The W film and the TaN film are both etched by on the sameorder by the second etching conditions using the gas mixture of CF₄ andCl₂. Note that the etching time may be increased on the order of 10 to20% in order to perform etching such that no residue remains on the gateinsulating film.

Edge portions of the first conductive layer and the second conductivelayer are made into a tapered shape in accordance with the effect of abias voltage, applied to the substrate side, by making the shapes of theresist masks suitable with the above-mentioned first etching condition.The angle of the tapered portions is from 15 to 45°. First shapeconductive layers 417 to 422 (first conductive layers 417 a to 422 a,and second conductive layers 417 b to 422 b) are thus formed from thefirst conductive layers and the second conductive layers by the firstetching process. Reference numeral 416 denotes a gate insulating film,and regions not covered by the first shape conductive layers 417 to 422become thinner by approximately 20 to 50 nm through etching.

A second etching process is then performed without removing the masksmade of resist (FIG. 12C). Here, W film is selectively etched by usingCF₄, Cl₂, and O₂ for the etching gas. At this time, the secondconductive layers 428 b to 433 b are formed by the second etchingprocess. On the other hand, the first conductive layers 417 a to 422 aare hardly etched and the second shape conductive layers 428 to 433 areformed.

A first doping process is then performed without removing the masks madeof resist and the semiconductor layer is added to the impurity elementwhich imparts n-type at a low concentration. The doping process may beperformed by ion doping method or ion injection method. Ion doping isperformed with process conditions in which the dosage is set from 1×10¹³to 5×10¹⁴/cm², and the acceleration voltage is set between 40 to 80 keV.Doping is performed in this embodiment with the dosage set to1.5×10¹³/cm², and the acceleration voltage set to 60 keV. An elementbelonging to the group 15, typically phosphorous (P) or arsenic (As) isused as an impurity element which imparts n-type. Phosphorous (P) isused here. In this case the conductive layers 428 to 433 act as maskswith respect to the impurity element which imparts n-type conductivity,and the impurity regions 423 to 427 are formed in a self-aligningmanner. The impurity element which imparts n-type is added to theimpurity regions 423 to 427 at a concentration in a range of 1×10¹⁸ to1×10²⁰/cm³.

Next, after removing the masks made of resist, new masks 434 a to 434 cmade of resist are formed, and the second doping process is performed inhigher acceleration voltage than the first doping process. Ion doping isperformed with process conditions in which the dosage is set from 1×10¹³to 1×10¹⁵/cm², and the acceleration voltage is set between 60 to 120keV. The doping process is performed by using the second conductivelayers 428 b to 432 b as masks and the semiconductor layer under thetapered portion of the first conductive layer is added to the impurityelement. Continuously the acceleration voltage is lowered than thesecond doping process, the third doping process is done, and the stateof FIG. 13A is obtained. Ion doping method is performed with processconditions in which the dosage is set from 1×10¹⁵ to 1×10¹⁷/cm², and theacceleration voltage is set between 50 to 100 keV. Low concentrationimpurity regions 436, 442 and 448 overlapping with the first conductivelayer are added to the impurity element, which imparts n-type within therange of the density of 1×10¹⁸ to 5×10¹⁹/cm² by the second dopingprocess and the third doping process and high concentration impurityregions 435, 441, 444 and 447 are added to the impurity element, whichimparts n-type within the range of the density of 1×10¹⁹ to 5×10²¹/cm².

Of course, the second doping process and the third doping process can beone-time doping processes by making it to a suitable accelerationvoltage and it is also possible to form the low concentration impurityregion and high concentration impurity region.

Next, after removing the masks made of resist, new masks 450 a to 450 cmade from resist are formed and the fourth doping process is performed.Impurity regions 453, 454, 459 and 460, to which an impurity elementwhich imparting a conductivity type opposite to that of the above oneconductivity type is added, are formed in accordance with the fourthdoping process in the semiconductor films which become active layers ofthe p-channel type TFTs. The first conductive layers 429 a to 432 a areused as masks with respect to the impurity element, and an impurityelement which imparts p-type conductivity is added to form the impurityregions in a self-aligning manner. The impurity regions 453, 454, 459and 460 are formed by ion doping method using diborane (B₂H₆) in thisembodiment (FIG. 13B). The semiconductor layers for forming then-channel type TFT are covered with the masks 450 a to 450 c made ofresist when the fourth doping process is performed. Phosphorous is addedat different concentrations into the impurity regions 453, 454, 459 and460 by the first to third doping processes. However, by performingdoping such that the concentration of the impurity element which impartsp-type conductivity becomes from 1×10¹⁹ to 5×10²¹ atoms/cm³ in therespective regions, no problems develop in making the regions functionas source regions and drain regions of the p-channel type TFT.

The impurity regions are thus formed in the respective semiconductorlayers by the steps up through this point.

A first interlayer insulating film 461 is formed next after removing themasks 450 a to 450 c made of resist. This first interlayer insulatingfilm 461 is formed from an insulating film containing silicon, having athickness of 100 to 200 nm, by using plasma CVD method or sputteringmethod. A silicon oxynitride film having a thickness of 150 nm is formedby plasma CVD method in this embodiment. The first interlayer insulatingfilm 461 is of course not limited to a silicon oxynitride film, andother insulating films containing silicon may also be used, as a singlelayer or a lamination structure.

Subsequently, a recovery of the crystallinity of the semiconductor layerand an activation of the impurity elements added to the respectivesemiconductor layers are performed by irradiating the laser beam, asshown in FIG. 13C. As the laser activation, the laser beam irradiates tothe semiconductor film by applying one of Embodiments 1 to 6 or byfreely combining with these embodiments. It is desirable that asolid-state laser of a continuous oscillation or a pulse oscillation, agas laser, or metallic laser is used. Note that, as the above-mentionedsolid-state laser, there may be given a YAG laser of a continuousoscillation or a pulse oscillation, a YVO₄ laser, a YLF laser, a YAlO₃laser, a Y₂O₃ laser a glass laser, a ruby laser, an alexandrite laser, aTi: sapphire laser, and the like. As the above-mentioned gas laser,there may be given a excimer laser of continuous oscillation or pulseoscillation, Ar laser, Kr laser, CO₂ laser, or the like. And as theabove-mentioned metallic laser, there may be given a helium cadmiumlaser, a copper vapor laser, or a gold vapor laser. At this moment, if acontinuous oscillation laser is used, about 0.01 to 100 MW/cm²(preferably 0.01 to 10 MW/cm²) is necessary for the energy density oflaser beam. The substrate is relatively moved to the laser beam at aspeed of about 0.5 to 2000 cm/s. And, if a pulse oscillation laser isused, it is desirable that 300 Hz of frequency and 50 to 1000 MJ/cm²(typically, 50 to 500 mJ/cm²) of laser energy density are used. At thismoment, laser beam may be overlapped by 50 to 98%. Besides laserannealing method, thermal annealing method or rapid thermal annealingmethod (RTA method) and the like can be applied.

Further, the activation may also be performed before the formation of afirst interlayer insulating film. However, if the wiring material usedis weak with respect to heat, then it is desirable to perform theactivation processing after forming an interlayer insulating film (aninsulating film having silicon as its main constituent, for example asilicon nitride film) in order to protect the wirings and the like, asin this embodiment.

Then, a heat treatment can also be performed (at 300 to 550° C. for 1 to12 hours) and it is possible to conduct a hydrogenation. This process isone of terminating dangling bonds in the semiconductor layers byhydrogen contained within the first interlayer insulating film 461. Thesemiconductor layers can be hydrogenated whether or not the firstinterlayer insulating film exists. Plasma hydrogenation (using hydrogenexcited by a plasma), and a heat treatment for 1 to 12 hours at atemperature of 300 to 450° C. in an atmosphere containing hydrogen offrom 3 to 100% may also be performed as other means of hydrogenation.

Subsequently, a second interlayer insulating film 462 made from aninorganic insulating film material or from an organic insulatingmaterial is formed on the first interlayer insulating film 461. Anacrylic resin film having a film thickness of 1.6 μm is formed in thisembodiment, and the material used may have a viscosity from 10 to 1000cp, preferably between 40 to 200 cp. A material in which unevenness isformed on its surface is used.

In order to prevent mirror reflection, the surface of a pixel electrodeis made uneven by forming a second interlayer insulating film whichforms an uneven surface (not shown) in this embodiment. Further, thepixel electrode surface can be made to be uneven and have lightscattering characteristics, and therefore a convex portion may also beformed in a region below the pixel electrode. The formation of theconvex portion can be performed by the same photomask as that forforming the TFTs, and therefore it can be formed without increasing thenumber of process steps. Note that the convex portion may also be formedappropriately on the substrate of the pixel portion region except thewirings and TFTs. In this way, unevenness is formed in the surface ofthe pixel electrode along the unevenness formed in the surface of theinsulating film which covers the convex portion.

A film having a level surface may also be used as the second interlayerinsulating film 462. In this case, it is desirable that the surface bemade uneven by an added process such as a known sandblasting process oretching process to prevent mirror reflection, and thereby increasingwhiteness by scattering reflected light.

Wirings 463 to 467 for electrically connecting respective impurityregions are then formed in a driver circuit 506. Note that a laminationfilm of a Ti film having a thickness of 50 nm and an alloy film (analloy of Al and Ti) having a thickness of 500 nm is patterned in orderto form the wirings. Of course, it is not limited to the two-layerstructure, the single-layer structure or the lamination structure morethan three layers may also be acceptable. Further, Al and Ti are notlimited to the wiring material. For example, Al and Cu are formed on TaNfilm, and the lamination film forming the Ti film is formed by thepatterning and form wiring (FIG. 14).

Further, a pixel electrode 470, a gate wiring 469, and a connectionelectrode 468 are formed in a pixel portion 507. An electricalconnection is formed with the pixel TFT and the source wiring(lamination of 433 a and 433 b) by the connection electrode 468.Further, the gate wiring 469 forms an electrical connection with thegate electrode of the pixel TFT. The pixel-electrode 470 forms anelectrical connection with the drain region 444 of the pixel TFT, and inaddition, forms an electrical connection with the semiconductor layer459 which functions as one electrode forming a storage capacitor. It isdesirable to use a material having superior reflectivity, such as a filmhaving Al or Ag as its main constituent, or a lamination film of suchfilms, as the pixel electrode 470.

A CMOS circuit composed of a n-channel TFT 501 and a p-channel TFT 502,a driver circuit 506 having a n-channel TFT 503, and the pixel portion507 having a pixel TFT 504 and a storage capacitor 505 can thus beformed on the same substrate. The active matrix substrate is thuscompleted.

The n-channel TFT 501 of the driver circuit 506 has: a channel formingregion 437; the low concentration impurity region 436 (GOLD region)which overlaps with the first conductive layer 428 a that structures aportion of the gate electrode; and the high concentration impurityregion 452 which functions as a source region or a drain region. Thep-channel TFT 502, which forms the CMOS circuit with the n-channel TFT501 and the electrode 466 by an electrical connection has: a channelforming region 455; the low concentration impurity region 454; and theimpurity region 453 in which the impurity elements imparting n-type andp-type are introduced. Further, the n-channel TFT 503 has: a channelforming region 443; the low concentration impurity region 442 (GOLDregion) which overlaps with the first conductive layer 430 a thatstructures a portion of the gate electrode; and the high concentrationimpurity region 456 which functions as a source region or a drainregion.

The pixel TFT 504 of the pixel portion has: a channel forming region446; the low concentration impurity region 445 (LDD region) formed onthe outside of the gate electrode; and the high concentration impurityregion 458 which functions as a source region or a drain region.Further, an impurity element which imparts n-type and an impurityelement which imparts p-type are added to the semiconductor layer whichfunctions as one electrode of the storage capacitor 505. The storagecapacitor 505 comprises an electrode (lamination of 432 a and 432 b) andthe semiconductor layer, with the insulating film 416 functioning as adielectric.

Edge portions of the pixel electrodes are disposed so as to overlap withsource wirings such that gaps between the pixel electrodes shield thelight, without using a black matrix, with the pixel structure of thisembodiment.

An upper surface diagram of the pixel portion of the active matrixsubstrate manufactured in this embodiment is shown in FIG. 15. Note thatthe same reference symbols are used for portions corresponding to thosein FIGS. 12 to 15. A chain line A-A′ in FIG. 14 corresponds to a crosssectional diagram cut along a chain line A-A′ within FIG. 15. Further, achain line B-B′ in FIG. 14 corresponds to a cross sectional diagram cutalong a chain line B-B′ within FIG. 15.

Embodiment 8

In this embodiment, a manufacturing process of a reflection type liquidcrystal display device from the active matrix substrate manufactured inaccordance with Embodiment 7 will be described hereinbelow. FIG. 16 isused for an explanation thereof.

First, in accordance with Embodiment 5, an active matrix substrate in astate shown in FIG. 14 is obtained, and thereafter, an alignment film567 is formed on the active matrix substrate of FIG. 14, at least on thepixel electrode 470, and is subjected to a rubbing process. Note that,in this embodiment, before the formation of the alignment film 567, aspacer 572 for maintaining a gap between the substrates is formed at adesired position by patterning an organic film such as an acrylic resinfilm. Further, spherical spacers may be scattered on the entire surfaceof the substrate in place of the columnar like spacer.

Next, an opposing substrate 569 is prepared. The colored layers 570, 571and a leveling film 573 are formed on the opposing substrate 569. Thered-colored layer 570 and the blue-colored layer 572 are partiallyoverlapped with each other, thereby forming a light shielding portion.Note that, the red-colored layer and a green-colored layer are partiallyoverlapped with each other, thereby forming a light shielding portion.

In this embodiment, the substrate shown in Embodiment 5 is used.Accordingly, in FIG. 15 showing a top view of the pixel portion inaccordance with Embodiment 5, light shielding must be performed at leastgaps between the gate wiring 469 and the pixel electrodes 470, a gapbetween the gate wiring 469 and the connection electrode 468, and a gapbetween the connection electrode 468 and the pixel electrode 470. Inthis embodiment, the opposing substrate and the active matrix substrateare stuck so that the light shielding portions from laminated layer ofcolored layer each other overlap with the positions which need to beshielded from light.

Like this, without forming a black matrix, the gaps between therespective pixels are shielded from light by the light shieldingportion. As a result, the reduction of the manufacturing steps can beattained.

Next, the opposing electrode 576 from transparent conductive film isformed on the leveling film 573, at least on the pixel portion. Thealignment film 574 on the entire surface of the opposing substrate andthe rubbing process is performed.

Then, an active matrix substrate on which a pixel portion and a drivercircuit are formed is stuck with the opposing substrate by a sealingagent 568. In the sealing agent 568, a filler is mixed, and the twosubstrates are stuck with each other while keeping a uniform gap by theeffect of this filler and the columnar spacer. Thereafter, a liquidcrystal material 575 is injected between both the substrates toencapsulate the substrates completely by an encapsulant (notillustrated). A known liquid crystal material may be used as the liquidcrystal material 575. Thus, the reflection type liquid crystal displaydevice shown in FIG. 16 is completed. Then, if necessary, the activematrix substrate or the opposing substrate may be parted into desiredshapes. Further, a polarizing plate is adhered to only the opposingsubstrate (not illustrated). Then, an FPC is adhered using a knowntechnique.

Thus formed liquid crystal display device have a TFT which is formed byusing the semiconductor film conducted homogeneous annealing. Therefore,enough operating characteristics and reliability of the above-mentionedliquid crystal display device can be obtained. Such liquid crystaldisplay device can be used as a display portion of various electronicdevice.

This embodiment can be combined with Embodiments 1 and 7 freely.

Embodiment 9

In this embodiment, the example of manufacturing the light-emittingdevice by using manufacturing method of TFT when forming the activematrix substrate shown in Embodiment 7 is described. In thisspecification, the light-emitting device is a generic name which is adisplay panel enclosing the light-emitting element between the substrateand the cover material and the display module mounted mounting an TFT onthe display panel. The light-emitting element has a light-emitting layercontaining an organic compound material which can obtain the electroluminescence generated by adding the electric field, the anode layer andthe cathode layer. Further, in the luminescence in an organic compound,the luminescence (fluorescence light) when returning from the state ofsinglet exciton to the basic state and the luminescence (phosphoruslight) when returning from the state of triplet exciton to the basicstate. Either or both luminescence are contained.

Further, in this embodiment, the organic light-emitting layer is definedall layers formed between the anode and the cathode. The organiclight-emitting layer is specifically including the light-emitting layer,the hole injection layer, the electron injection layer, the holetransport layer, the electron transport layer and the like. Basically,the light-emitting element have a structure which is constructed by theanode layer, the light-emitting layer and the cathode layersequentially. Additionally, the light-emitting layer may have followingtwo structures. The first structure is constructed sequentially by theanode layer, the hole injection layer, the light-emitting layer and thecathode layer. The second structure is sequentially constructed by theanode layer, the hole injection layer, the light-emitting layer, theelectron injection layer, the cathode layer and the like.

FIG. 17 is a cross-sectional view of the light-emitting device of thepresent invention. In FIG. 17, a switching TFT 603 provided on asubstrate 700 is formed using the n-channel type TFT 503 of FIG. 17.Thus, this structure may be referred to the description of the n-channeltype TFT 503.

Note that, in this embodiment, a double gate structure in which twochannel forming regions are formed is used. However, a single gatestructure in which one channel forming region is formed, or a triplegate structure in which three channel forming regions are formed may beused.

A driver circuit provided on the substrate 700 is formed using the CMOScircuit of FIG. 14. Thus, this structure may be referred to thedescriptions of the n-channel type TFT 501 and the p-channel type TFT502. Note that, in this embodiment, the single gate structure is used.However, the double gate structure or the triple gate structure may alsobe used.

Also, wirings 701 and 703 function as a source wiring of the CMOScircuit, a wiring 702 functions as a drain wiring thereof. A wiring 704functions as a wiring for electrically connecting a source wiring 708with a source region of the switching TFT. A wiring 705 functions as awiring for electrically connecting a drain wiring 709 with a drainregion of the switching TFT.

Note that, a current-controlled TFT 604 is formed using the p-channeltype TFT 502 of FIG. 14. Thus, this structure may be referred to thedescriptions of the p-channel type TFT 502. Note that, in thisembodiment, the single gate structure is used. However, the double gatestructure or the triple gate structure may be used.

Also, a wiring 706 is a source wiring (corresponding to a current supplyline) of the current-controlled TFT 604 and a wiring 707 is a drainwiring of the current-controlled TFT 604. Reference numeral 707 denotesan electrode which is electrically connected with a pixel electrode 711by overlapping with the pixel electrode 711 of the current-controlledTFT 604.

Note that, reference numeral 711 denotes the pixel electrode (anode of alight-emitting element) made from a transparent conductive film. As thetransparent conductive film, a compound of indium oxide and tin oxide, acompound of indium oxide and zinc oxide, zinc oxide, tin oxide, orindium oxide can be used. Also, the above-mentioned transparentconductive film to which gallium is added may be used. The pixelelectrode 711 is formed on a level interlayer insulating film 710 beforethe formation of the above wirings. In this embodiment, it is veryimportant to level a step in the TFT using the leveling film 710 made ofresin. Since a light-emitting layer formed later is extremely thin,there is the case where insufficient light-emitting occurs due to thestep. Thus, in order to form the light-emitting layer as level aspossible, it is desired that the step is leveled before the formation ofthe pixel electrode 711.

After the wirings 701 to 707 are formed, a bank 712 is formed as shownin FIG. 17. The bank 712 may be formed by patterning an insulating filmwith a thickness of 100 to 400 nm containing silicon or an organic resinfilm.

Note that, since the bank 712 is an insulating film, it is necessary topay attention to a dielectric breakdown of an element in the filmformation. In this embodiment, a carbon particle or a metal particle isadded to the insulating film which is a material of the bank 712 toreduce a resistivity. Thus, an electrostatic occurrence is suppressed.Here, an additional amount of the carbon particle or the metal particlemay be controlled such that the resistivity is 1×10⁶ to 1×10¹² Ωm(preferably, 1×10⁸ to 1×10¹⁰ Ωm).

A light emitting layer 713 is formed on the pixel electrode 710. Notethat, only one pixel is shown in FIG. 17. However, in this embodiment,the light-emitting layers are formed corresponding to respective colorsof R (red), G (green), and B (blue). Also, in this embodiment, a lowmolecular organic light-emitting material is formed by an evaporationmethod. Concretely, copper phthalocyanine (CuPc) film with a thicknessof 20 nm is provided as a hole injection layer, and atris-8-quinolinolate aluminum complex (Alq₃) film with a thickness of 70nm is provided thereon as a light-emitting layer. Thus, a laminationstructure of those films is formed. A light-emitting color can becontrolled by adding a fluorochrome such as quinacridon, perylene, orDCM1 to Alq₃.

Note that, the above example is one example of the organiclight-emitting material which can be used as the light-emitting layer,and it is unnecessary to be limited to this example. The light-emittinglayer (layer for causing light to emit and a carrier to move for theemitting of light) may be formed by freely combining the light-emittinglayer and a charge transport layer or a charge injection layer. Forexample, in this embodiment, although the example that the low molecularorganic light-emitting material is used as the light-emitting layer isshown, intermediate molecular-weight organic light emitting material ora polymer organic light-emitting material may be also used. Furthermore,an organic light-emitting material having no sublimation property buthaving molecules in the number of 20 or less or chained molecules havinga length of 10 μm or less, is provided as a intermediate molecularorganic light emitting material. For an example of using the highmolecular weight organic light emitting material, a polythiophene(PEDOT) film with a thickness of 20 nm is formed by the spin coatingmethod as a hole injection layer and the lamination structure installingparaphenylenvinylene (PPV) of about 100 nm on it as a light emittinglayer may be good. The luminescence wave length can be selected from redto blue by using the π-conjugated type polymer of PPV. Meanwhile, it ispossible to use an inorganic material such as silicon carbide for anelectron transporting layer or charge injecting layer. These organiclight emitting materials or inorganic materials can be a known material.

Next, a cathode 714 made from a conductive film is provided on thelight-emitting layer 713. In the case of this embodiment, an alloy filmof aluminum and lithium is used as the conductive film. Of course, aknown MgAg film (alloy film of magnesium and silver) may be used. As acathode material, the conductive film made of an element which belongsto group 1 or group 2 of the periodic table, or the conductive film towhich those elements are added may be used.

When this cathode 714 is formed, a light-emitting element 715 iscompleted. Note that, the light-emitting element 715 completed hererepresents a diode formed by the pixel electrode (anode) 711, thelight-emitting layer 713, and the cathode 714.

It is effective to provide a passivation film 716 so as to completelycover the light-emitting element 715. As the passivation film 716, asingle layer of an insulating film containing a carbon film, a siliconnitride film, or silicon oxynitride film, or a lamination layer of acombination with the insulating film is used.

Here, it is preferred that a film with a good coverage is used as thepassivation film, and it is effective to use the carbon film, inparticular a DLC (diamond like carbon) film. Since the DLC film can beformed in a range of a room temperature to 100° C., it can be easilyformed over the light-emitting layer 713 with a low heat-resistance.Also, since the DLC film has a high blocking effect against oxygen, theoxidation of the light-emitting layer 713 can be suppressed. Thus, theoxidation of the light-emitting layer 713 during the following sealingprocess can be prevented.

Further, a sealing member 717 is provided on the passivation film 716,and then a cover member 718 is adhered to the sealing member 717.Ultraviolet light cured resin may be used as the sealing member 717, andit is effective to provide a material having a hygroscopic effect or amaterial having an oxidation inhibition effect inside. Also, in thisembodiment, a member in which a carbon film (preferably, a diamondcarbon like film) is formed on both surfaces of, a glass substrate, aquartz substrate, or a plastic substrate (including a plastic film) isused as the cover member 718. Aluminum film (AlON, AlN, AlO and thelike), SiN and the like can be used instead of a carbon film.

Thus, a light-emitting device of the structure as shown in FIG. 17 iscompleted. Note that, after the formation of the bank 712, it iseffective to successively perform the processes until the formation ofthe passivation film 716 using a film formation apparatus of a multichamber system (or an inline system) without exposing to air. Further,processes until the adhesion of the cover member 718 can be successivelyperformed without exposing to air.

Thus, n-channel TFT 601, p-channel TFT 602, a switching TFT (n-channelTFT) 603, and a current control TFT (p-channel TFT) 604 are formed onthe substrate 700.

Further, as described using FIG. 17, when the impurity regionsoverlapped with the gate electrode through the insulating film areprovided, the n-channel TFT having a high resistant against thedeterioration due to a hot carrier effect can be formed. Thus, thelight-emitting device with high reliability can be realized.

In this embodiment, only the structures of the pixel portion and thedriver circuit are shown. However, according to the manufacturingprocess of this embodiment, logic circuits such as a signal separationcircuit, a D/A converter, an operational amplifier, a γ-correctioncircuit and the like can be further formed on the same insulatingmaterial. A memory and a microprocessor can be also formed.

Thus formed light-emitting device have a TFT which is formed by usingthe semiconductor film conducted homogeneous annealing. Therefore,enough operating characteristics and reliability of the above-mentionedlight-emitting device can be obtained. Such light-emitting device can beused as a display portion of various electronic devices.

This embodiment can be performed by freely combining with Embodiments 1to 7.

Embodiment 10

Various semiconductor devices (active matrix type liquid crystal displaydevice, active matrix type light-emitting device or active matrix typeEC display device) can be formed by applying the present invention.Specifically, the present invention can be embodied in electroopticsequipment of any type in which such an electrooptical device isincorporated in a display portion.

Such electronic equipment is a video camera, a digital camera, aprojector, a head-mounted display (goggle type display), a carnavigation system, a car stereo, a personal computer, or a mobileinformation terminal (such as a mobile computer, a mobile telephone, anelectronic book and the like). FIGS. 18A-18F, 19A-19D, and 20A-20C showone of its examples.

FIG. 18A shows a personal computer which includes a body 3001, an imageinput portion 3002, a display portion 3003, a keyboard 3004 and thelike. A personal computer completes by applying the semiconductor devicethat applies this invention to display portion 3003.

FIG. 18B shows a video camera which includes a body 3101, a displayportion 3102, a sound input portion 3103, operating switches 3104, abattery 3105, an image receiving portion 3106 and the like. A videocamera completes by applying the semiconductor device that applies thisinvention to display portion 3102.

FIG. 18C shows a mobile computer which includes a body 3201, a cameraportion 3202, an image receiving portion 3203, an operating switch 3204,a display portion 3205 and the like. A mobile computer completes byapplying the semiconductor device that applies this invention to displayportion 3205.

FIG. 18D shows a goggle type display which includes a body 3301, adisplay portion 3302, arm portions 3303 and the like. A goggle typedisplay completes by applying the semiconductor device that applies thisinvention to display portion 3302.

FIG. 18E shows a player using a recording medium on which a program isrecorded (hereinafter referred to as the recording medium), and theplayer includes a body 3401, a display portion 3402, speaker portions3403, a recording medium 3404, operating switches 3405 and the like.This player uses a DVD (Digital Versatile Disc), a CD and the like asthe recording medium, and enables a user to enjoy music, movies, gamesand the Internet. A recording medium completes by applying thesemiconductor device that applies this invention to display portion3402.

FIG. 18F shows a digital camera which includes a body 3501, a displayportion 3502, an eyepiece portion 3503, operating switches 3504, animage receiving portion (not shown) and the like. A digital cameracompletes by applying the semiconductor device that applies thisinvention to display portion 3502.

FIG. 19A shows a front type projector which includes a projection device3601, a screen 3602 and the like. A front type projector completes byapplying the semiconductor device that applies this invention to aliquid crystal display device 3808 composing a part of a projectiondevice 3601 as well as other driver circuit.

FIG. 19B shows a rear type projector which includes a body 3701, aprojection device 3702, a mirror 3703, a screen 3704 and the like. Arear type projector completes by applying the semiconductor device thatapplies this invention to a liquid crystal display device 3808 composinga part of a projection device 3702 as well as other driver circuit.

FIG. 19C shows one example of the structure of each of the projectiondevices 3601 and 3702 which are respectively shown in FIGS. 19A and 19B.Each of the projection devices 3601 and 3702 is made of a light sourceoptical system 3801, mirrors 3802 and 3804-3806, a dichroic mirror 3803,a prism 3807, a liquid crystal display device 3808, a phase differenceplate 3809 and a projection optical system 3810. The projection opticalsystem 3810 is made of an optical system including a projection lens.Embodiment 10 is an example of a three-plate type, but it is not limitedto this example and may also be of a single-plate type. In addition,those who embody the invention may appropriately dispose an opticalsystem such as an optical lens, a film having a polarization function, afilm for adjusting phase difference or an IR film in the path indicatedby arrows in FIG. 19C.

FIG. 19D is a view showing one example of the structure of the lightsource optical system 3801 shown in FIG. 19C. In Embodiment 10, thelight source optical system 3801 is made of a reflector 3811, a lightsource 3812, lens arrays 3813 and 3814, a polarizing conversion element3815 and a condenser lens 3816. Incidentally, the light source opticalsystem shown in FIG. 19D is one example, and the invention is notparticularly limited to the shown construction. For example, those whoembody the invention may appropriately dispose an optical system such asan optical lens, a film having a polarization function, a film foradjusting phase difference or an IR film.

The projector shown in FIGS. 19A to 19D is of the type using atransparent type of electrooptical device, but there is not shown anexample in which the invention is applied to a reflection type ofelectrooptical device and a light-emitting device.

FIG. 20A shows a cell phone which includes a body 3901, a sound outputportion 3902, a sound input portion 3903, a display portion 3904,operating switches 3905, an antenna 3906 and the like. A cell phonecompletes by applying the semiconductor device that applies thisinvention to display portion 3904.

FIG. 20B shows a mobile book (electronic book) which includes body 4001,display portions 4002 and 4003, a storage medium 4004, operatingswitches 4005, an antenna 4006 and the like. A mobile book completes byapplying the semiconductor device that applies this invention to displayportion 4002 and 4003.

FIG. 20C shows a display which includes a body 4101, a support base4102, a display portion 4103 and the like. A display completes byapplying the semiconductor device that applies this invention to displayportion 4103. The invention is particularly advantageous to alarge-screen display, and is advantageous to a display having a diagonalsize of 10 inches or more (particularly, 30 inches or more).

As is apparent from the foregoing description, the range of applicationsof the invention is extremely wide, and the invention can be applied toany category of electronic apparatus. Electronic apparatus according tothe invention can be realized by using a construction made of acombination of arbitrary ones of Embodiments 1 to 8 and 9.

Employing the structures of the present invention provides the followingbasic usefulness:

-   a) Laser light very excellent in uniformity of energy distribution    can be formed on an irradiation surface or in the vicinity thereof    and accordingly an irradiation object can be annealed uniformly.-   b) Laser beams emitted from different lasers are synthesized and    therefore interference does not take place, and this is effective    especially when highly interferential lasers are used.-   c) The throughput can be improved, which is effective particularly    when a substrate has a large area.-   d) With those advantages given in the above, the present invention    can improve the operation characteristic and reliability of    semiconductor devices, typically, active matrix liquid crystal    display devices, and can lower manufacture cost of semiconductor    devices.

What is claimed is:
 1. A laser irradiation apparatus comprising: aplurality of lasers; means for cutting each of plural first laser lightspots emitted from the plural lasers to divide the plural first laserlight spots into plural second laser light spots; and means for choosingone laser light spot out of the second laser light spots for each of theplural first laser light spots and synthesizing the chosen laser lightspots in the same region on an irradiation surface.
 2. A laserirradiation apparatus comprising: a plurality of lasers; means forcutting each of plural first laser light spots emitted from the plurallasers to divide the plural first laser light spots into plural secondlaser light spots; and means for choosing one laser light spot out ofthe second laser light spots for each of the plural first laser lightspots and synthesizing the chosen laser light spots in the same regionon an irradiation surface, the chosen laser light spots having differentenergy distributions from one another.
 3. A laser irradiation apparatusaccording to claim 1, wherein laser light formed by synthesizing spotsin the same region on the irradiation surface has a linear shape.
 4. Alaser irradiation apparatus according to claim 2, wherein laser lightformed by synthesizing spots in the same region on the irradiationsurface has a linear shape.
 5. A laser irradiation apparatus accordingto claim 1, wherein the choosing and synthesizing means is one or morekinds selected from a mirror and a cylindrical lens.
 6. A laserirradiation apparatus according to claim 2, wherein the synthesizingmeans is one or more kinds selected from a mirror and a cylindricallens.
 7. A laser irradiation apparatus comprising: a plurality oflasers; means for cutting each of plural first laser light spots emittedfrom the plural lasers to divide the plural first laser light spots intoplural second laser light spots; a convex lens placed at an angle to theplural second laser light spots; and means for choosing one laser lightspot out of the second laser light spots that have exited the convexlens for each of the plural first laser light spots and synthesizing thechosen laser light spots in the same region on an irradiation surface,wherein the irradiation surface is placed such that laser light that haspassed through the convex lens enters the irradiation surface at anangle, and wherein the laser light has a linear shape on the irradiationsurface because of the convex lens.
 8. A laser irradiation apparatuscomprising: a plurality of lasers; means for cutting each of pluralfirst laser light spots emitted from the plural lasers to divide theplural first laser light spots into plural second laser light spots; aconvex lens placed at an angle to the plural second laser light spots;and means for choosing one laser light spot out of the second laserlight spots that have exited the convex lens for each of the pluralfirst laser light spots and synthesizing the chosen laser light spots inthe same region on an irradiation surface, the chosen laser light spotshaving different energy distributions from one another, wherein theirradiation surface is placed such that laser light that has passedthrough the convex lens enters the irradiation surface at an angle, andwherein the laser light has a linear shape on the irradiation surfacebecause of the convex lens.
 9. A laser irradiation apparatus accordingto claim 7, wherein, when the beam length of the laser light entering anirradiation object set on a substrate is given as w₁, the beam length ofa part of the laser light that is reflected at the back side of thesubstrate is given as w₂, thickness of the substrate is given as d, andw=(w₁+w₂)/2, an incident angle θ of the laser light entering theirradiation object satisfies θ≧arctan(W/(2×d)).
 10. A laser irradiationapparatus according to claim 8, wherein, when the beam length of thelaser light entering an irradiation object set on a substrate is givenas w₁, the beam length of a part of the laser light that is reflected atthe back side of the substrate is given as w₂, the thickness of thesubstrate is given as d, and w=(w₁+w₂)/2, an incident angle θ of thelaser light entering the irradiation object satisfies θ≧arctan(W/(2×d)).11. A laser irradiation apparatus according to claim 7, wherein theincident angle θ of the laser light entering the irradiation object isBrewster angle.
 12. A laser irradiation apparatus according to claim 8,wherein the incident angle θ of the laser light entering the irradiationobject is Brewster angle.
 13. A laser irradiation apparatus according toclaim 1, wherein the dividing means is one or more kinds selected from aslit, a mirror, a prism, a cylindrical lens, and a cylindrical lensarray.
 14. A laser irradiation apparatus according to claim 2, whereinthe dividing means is one or more kinds selected from a slit, a mirror,a prism, a cylindrical lens, and a cylindrical lens array.
 15. A laserirradiation apparatus according to claim 7, wherein the dividing meansis one or more kinds selected from a slit, a mirror, a prism, acylindrical lens, and a cylindrical lens array.
 16. A laser irradiationapparatus according to claim 8; wherein the dividing means is one ormore kinds selected from a slit, a mirror, a prism, a cylindrical lens,and a cylindrical lens array.
 17. A laser irradiation apparatusaccording to claim 1, wherein each of the lasers is a continuous wave orpulse oscillation solid-body laser, gas laser, or metal laser.
 18. Alaser irradiation apparatus according to claim 2, wherein each of thelasers is a continuous wave or pulse oscillation solid-body laser, gaslaser, or metal laser.
 19. A laser irradiation apparatus according toclaim 7, wherein each of the lasers is a continuous wave or pulseoscillation solid-body laser, gas laser, or metal laser.
 20. A laserirradiation apparatus according to claim 8, wherein each of the lasersis a continuous wave or pulse oscillation solid-body laser, gas laser,or metal laser.
 21. A laser irradiation apparatus according to claim 1,wherein each of the lasers is selected from the group consisting of acontinuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser.
 22. A laser irradiation apparatus according to claim2, wherein each of the lasers is selected from the group consisting of acontinuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser.
 23. A laser irradiation apparatus according to claim7, wherein each of the lasers is selected from the group consisting of acontinuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser.
 24. A laser irradiation apparatus according to claim8, wherein each of the lasers is selected from the group consisting of acontinuous wave or pulse oscillation YAG laser, YVO₄ laser, YLF laser,YAlO₃ laser, Y₂O₃ laser, glass laser, ruby laser, alexandrite laser, andTi:sapphire laser.
 25. A laser irradiation apparatus according to claim1, wherein each of the lasers is selected from the group consisting ofan Ar laser, Kr laser, and CO₂ laser.
 26. A laser irradiation apparatusaccording to claim 2, wherein each of the lasers is selected from thegroup consisting of an Ar laser, Kr laser, and CO₂ laser.
 27. A laserirradiation apparatus according to claim 7, wherein each of the lasersis selected from the group consisting of an Ar laser, Kr laser, and CO₂laser.
 28. A laser irradiation apparatus according to claim 8, whereineach of the lasers is selected from the group consisting of an Ar laser,Kr laser, and CO₂ laser.
 29. A laser irradiation apparatus according toclaim 1, wherein each of the lasers is selected from the groupconsisting of a continuous wave or pulse oscillation helium cadmiumlaser, copper steam laser, and gold steam laser.
 30. A laser irradiationapparatus according to claim 2, wherein each of the lasers is selectedfrom the group consisting of a continuous wave or pulse oscillationhelium cadmium laser, copper steam laser, and gold steam laser.
 31. Alaser irradiation apparatus according to claim 7, wherein each of thelasers is selected from the group consisting of a continuous wave orpulse oscillation helium cadmium laser, copper steam laser, and goldsteam laser.
 32. A laser irradiation apparatus according to claim 8,wherein each of the lasers is selected from the group consisting of acontinuous wave or pulse oscillation helium cadmium laser, copper steamlaser, and gold steam laser.
 33. A laser irradiation apparatus accordingto claim 1, wherein each of the plurality of lasers emits laser lightwhich has been converted into harmonic by a non-linear optical element.34. A laser irradiation apparatus according to claim 2, wherein each ofthe plurality of lasers emits laser light which has been converted intoharmonic by a non-linear optical element.
 35. A laser irradiationapparatus according to claim 7, wherein each of the plurality of lasersemits laser light which has been converted into harmonic by a non-linearoptical element.
 36. A laser irradiation apparatus according to claim 8,wherein each of the plurality of lasers emits laser light which has beenconverted into harmonic by a non-linear optical element.
 37. A laserirradiation method comprising: emitting a first laser beam from a firstlaser; dividing the first laser beam into at least two divided firstlaser beams; emitting a second laser beam from a second laser; dividingthe second laser beam into at least two divided second laser beams;synthesizing one of the two divided first laser beams and one of the twodivided second laser beams to form a synthesized laser beam; andirradiating a surface with the synthesized laser beam.
 38. The laserirradiation method according to claim 37 wherein the surface is asurface of a semiconductor film.
 39. The laser irradiation methodaccording to claim 37 wherein the semiconductor film is crystallized bythe irradiation of the synthesized laser beam.